JPH03204592A - Heat exchanger - Google Patents
Heat exchangerInfo
- Publication number
- JPH03204592A JPH03204592A JP9190A JP9190A JPH03204592A JP H03204592 A JPH03204592 A JP H03204592A JP 9190 A JP9190 A JP 9190A JP 9190 A JP9190 A JP 9190A JP H03204592 A JPH03204592 A JP H03204592A
- Authority
- JP
- Japan
- Prior art keywords
- tube
- unit elements
- spiral
- heat exchanger
- helical element
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Pending
Links
- 239000007788 liquid Substances 0.000 claims abstract description 31
- 238000005219 brazing Methods 0.000 claims description 3
- 230000033001 locomotion Effects 0.000 abstract 1
- 230000000052 comparative effect Effects 0.000 description 17
- 238000010438 heat treatment Methods 0.000 description 14
- 239000006188 syrup Substances 0.000 description 9
- 235000020357 syrup Nutrition 0.000 description 9
- 229920002472 Starch Polymers 0.000 description 7
- 235000019698 starch Nutrition 0.000 description 7
- 239000008107 starch Substances 0.000 description 7
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 description 7
- 238000001816 cooling Methods 0.000 description 6
- 239000012530 fluid Substances 0.000 description 6
- 239000008399 tap water Substances 0.000 description 6
- 235000020679 tap water Nutrition 0.000 description 6
- 230000003068 static effect Effects 0.000 description 5
- 230000000694 effects Effects 0.000 description 4
- 230000005465 channeling Effects 0.000 description 2
- 238000004519 manufacturing process Methods 0.000 description 2
- 238000005259 measurement Methods 0.000 description 2
- -1 31G Substances 0.000 description 1
- 229920002261 Corn starch Polymers 0.000 description 1
- 239000002253 acid Substances 0.000 description 1
- 238000013019 agitation Methods 0.000 description 1
- 239000000919 ceramic Substances 0.000 description 1
- 239000000498 cooling water Substances 0.000 description 1
- 229910052802 copper Inorganic materials 0.000 description 1
- 239000008120 corn starch Substances 0.000 description 1
- 229940099112 cornstarch Drugs 0.000 description 1
- 230000005484 gravity Effects 0.000 description 1
- 238000005304 joining Methods 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 239000002184 metal Substances 0.000 description 1
- 230000000704 physical effect Effects 0.000 description 1
- 229920006395 saturated elastomer Polymers 0.000 description 1
- HBMJWWWQQXIZIP-UHFFFAOYSA-N silicon carbide Chemical compound [Si+]#[C-] HBMJWWWQQXIZIP-UHFFFAOYSA-N 0.000 description 1
- 229910010271 silicon carbide Inorganic materials 0.000 description 1
- 238000010998 test method Methods 0.000 description 1
Landscapes
- Heat-Exchange Devices With Radiators And Conduit Assemblies (AREA)
Abstract
Description
【発明の詳細な説明】
[産業上の利用分野コ
本発明は内管内に螺旋体を備えた内外管からなり、内管
と外管との間で流体(特に液体)の熱交換を行なう熱交
換器に関する。[Detailed Description of the Invention] [Industrial Field of Application] The present invention is a heat exchanger that is composed of an inner and outer tube with a spiral body inside the inner tube, and that exchanges heat of a fluid (particularly a liquid) between the inner tube and the outer tube. Concerning vessels.
[従来技術及び課題]
従来の熱交換器においては、熱交換率を向上させるため
多数の伝熱フィンやバッフルプレートを備えたものがあ
る。しかし、この種の熱交換器では、流体が層状に流れ
るいわゆるチャンネリング現象を生じ、熱交換向上の点
で限界ある。[Prior Art and Problems] Some conventional heat exchangers are equipped with a large number of heat transfer fins and baffle plates in order to improve heat exchange efficiency. However, in this type of heat exchanger, a so-called channeling phenomenon occurs in which the fluid flows in a layered manner, and there is a limit in terms of improving heat exchange.
又、内管内に 180°捻りのバッフルプレートを90
″接続角をもって逆向きに交互に接続した。いわゆるス
タティックミキサを用いることも行なわれている。しか
し、この場合接続部が多い等との関係で構造が極めて複
雑であり、製造上多大の工数を要する。そのため、多数
の内管を配設したり、長大管を使用して大きな伝熱面積
をとる必要がある場合、特にこの問題が支障となる。更
に圧力損失が大きく、省エネルギの見地からも課題があ
る。In addition, a 90° baffle plate with a 180° twist is installed inside the inner tube.
``Connections are made alternately in opposite directions with connection angles. A so-called static mixer is also used. However, in this case, the structure is extremely complicated due to the large number of connection parts, and it requires a large amount of man-hours in manufacturing. Therefore, this problem is particularly problematic when it is necessary to install a large number of inner pipes or use long and large pipes to secure a large heat transfer area.Furthermore, the pressure loss is large, and from the standpoint of energy saving, There are also challenges.
[解決手段及び効果コ
そこで2本発明は従来のスタティックミキサを用いた熱
交換器と同等の伝熱特性を有し、かつ上記課題を解決す
るために下記手段を採用した。[Solution Means and Effects] Therefore, the present invention employs the following means in order to have heat transfer characteristics equivalent to those of a conventional heat exchanger using a static mixer and to solve the above problems.
管内において長手方向に延びる螺旋エレメントを備え。Includes a helical element extending longitudinally within the tube.
螺旋エレメントが、捻り角度180°を有する複数の単
位エレメントを接続角度O0で連続してなり。The helical element consists of a plurality of unit elements each having a twist angle of 180° and connected at a connection angle O0.
隣接する単位エレメントが逆方向の捻りになっている。Adjacent unit elements are twisted in opposite directions.
ことを特徴とする熱交換用管体。A heat exchange tube body characterized by:
この熱交換用管体を内管とし、該一又は二以上の内管を
外管内に空隙をもって配設すれば、熱交換器の主要部が
構成される。If this heat exchange tube body is used as an inner tube and one or more inner tubes are disposed within the outer tube with a gap, the main part of the heat exchanger is constituted.
こうした手段によれば、スタティックミキサを利用した
ものに比して、極めて簡単な構造であり、しかも後述す
る実施例の試験結果から明らかにされるように、同等の
伝熱効果を達成できる。According to such means, the structure is extremely simpler than that using a static mixer, and, as will be made clear from the test results of the examples described later, it is possible to achieve the same heat transfer effect.
加えて、圧力損失が格段に低いので、省エネルギの見地
から好ましく、特に長大管等の熱交換器において、又低
粘性液体に対しこの効果が顕著であり、実用上の利点が
大きい。In addition, since the pressure loss is extremely low, it is preferable from the viewpoint of energy saving, and this effect is particularly noticeable in heat exchangers such as long and large pipes, and with low viscosity liquids, and has a great practical advantage.
[好適な手段]
熱交換用媒体としては液体、特にRe > 104の低
粘性液体例えば水に対して有効である。液体に特有な熱
交換時の難点(チャンネリング現象)も殆んど生じない
。[Preferred Means] The heat exchange medium is effective for liquids, especially low viscosity liquids with Re > 104, such as water. Difficulties during heat exchange (channeling phenomenon) peculiar to liquids also hardly occur.
管内壁との螺旋エレメントの接合は、ろう付が好ましい
。容易に接合でき高伝熱効率を確保できる。尚、この接
合によって内管の補強にもなりその肉厚を薄くしてもた
わみが少なく、その公吏に伝熱効率増大に資する。The helical element is preferably joined to the inner wall of the pipe by brazing. It can be easily joined and high heat transfer efficiency can be ensured. Furthermore, this joining also serves to reinforce the inner tube, and even if its wall thickness is made thinner, there is less deflection, which contributes to increasing the heat transfer efficiency of the tube.
上記螺旋エレメントによれば逆捩り攪拌の効果が付与さ
れ、内外管の空隙内のバッフルは必ずしも要しない。The spiral element described above provides the effect of reverse torsional agitation, and does not necessarily require baffles in the gaps between the inner and outer tubes.
−の螺旋エレメントを構成する単位エレメントの数は用
途に応じて適宜選択される。又、螺旋エレメントは単位
エレメントを製造した後、溶接。The number of unit elements constituting the spiral element - is appropriately selected depending on the application. In addition, the spiral element is welded after manufacturing the unit element.
ロウ付するか、或いは当初より一体のものとして製造す
る。It can be soldered or manufactured as one piece from the beginning.
尚、各単位エレメント(捻り角 180°)の長手力向
長さ(L)の内管内径(D>に対する比(1−、/ D
)は1通常のスタティックミキサの単位エレメントと
同様に、1〜3程度が好ましい。In addition, the ratio (1-, / D
) is preferably about 1 to 3, similar to the unit element of a normal static mixer.
[実施例]
第1A図は本実施例に係る螺旋エレメント1を示し、該
螺旋エレメント1は捻り角度180°の複数(図では4
)の単位エレメント1a・・からなり単位エレメント毎
に捩り方向が逆向き、かつ接続角度O0をもって連結さ
れている。そのため。[Example] FIG. 1A shows a helical element 1 according to this example, and the helical element 1 has a plurality of twist angles of 180° (4 in the figure).
), each unit element is twisted in the opposite direction and connected at a connection angle O0. Therefore.
螺旋エレメント1は管内において長手方向に延びる連続
したーの螺旋シートとして存在する。この点 従来の典
型的なスタティックミキサのエレメントが、単位エレメ
ントが相互に接続角度(例えば90°)をもって不連続
に接続されている構成(第1B図)とは全く相違する。The helical element 1 is present in the tube as a continuous helical sheet extending longitudinally. In this respect, the elements of a typical conventional static mixer are completely different from the structure (FIG. 1B) in which unit elements are discontinuously connected to each other at a connection angle (for example, 90 degrees).
従って1本例(本発明)の螺旋エレメント1は管内に配
備されたとき、管を二のチャンネルに分割するだけであ
る。Thus, when the helical element 1 of one example (invention) is deployed in a pipe, it only divides the pipe into two channels.
螺旋エレメント1 (単位エレメント1a・・・)は、
内管内を流れる液体の種類・圧力に応じ、好ましくは良
好な熱伝導性を有する材料1例えば5S41.5LIS
31G、 Cu 、 N i等の金属、又は炭化珪素
等のセラミックスで構成される。螺旋エレメント1と管
内壁とはろう付けで接合され、−保父されている。The spiral element 1 (unit element 1a...) is
Depending on the type and pressure of the liquid flowing inside the inner tube, it is preferable to use a material 1 having good thermal conductivity, such as 5S41.5LIS.
It is made of a metal such as 31G, Cu, or Ni, or a ceramic such as silicon carbide. The helical element 1 and the inner wall of the tube are joined by brazing and held together.
この螺旋エレメント1を備えた熱交換器Aを第1−1図
に示す。同図において、2は内管、3は外管である。本
例は4本の内管2・・・を備えた例を示している。A heat exchanger A equipped with this spiral element 1 is shown in FIG. 1-1. In the figure, 2 is an inner tube, and 3 is an outer tube. This example shows an example including four inner tubes 2.
係る構成の熱交換器Aにおいて、熱交換用液体を矢印方
向に流入させると、二のチャンネルに分割され、各チャ
ンネルにおいて1分割液体は各単位エレメント1a・・
・によって螺旋運動しながら。In the heat exchanger A having such a configuration, when the heat exchange liquid is allowed to flow in the direction of the arrow, it is divided into two channels, and in each channel, one divided liquid is distributed to each unit element 1a...
・While moving in a spiral manner.
かつ単位エレメント1a毎に逆捩すしながら長手方向に
移動することとなる。In addition, each unit element 1a moves in the longitudinal direction while being reversely twisted.
[試験] (1)目的 本実施例の熱交換器の性能を確認する。[test] (1) Purpose The performance of the heat exchanger of this example will be confirmed.
比較例として、従来の標準エレメント(図IB)を備え
てなる熱交換器を用いた。尚、参考のため、空管(図I
C)の熱交換器についても調べた。As a comparative example, a heat exchanger equipped with a conventional standard element (FIG. IB) was used. For reference, an empty tube (Figure I
The heat exchanger C) was also investigated.
(2)試験装置および試験方法 試験に用いた熱交換フローを図1−2に示す。(2) Test equipment and test method The heat exchange flow used in the test is shown in Figure 1-2.
図1−2においてrFIJは流量指示計、「P」は圧力
、rP、Jは蒸気圧力、そしてrT I Clは温度指
示調整計を夫々示す。また熱交換器の仕様を表1に示す
。尚、螺旋エレメントの全長(L)はいずれも810m
mとした。In FIG. 1-2, rFIJ indicates a flow rate indicator, "P" indicates pressure, rP, J indicates steam pressure, and rT I Cl indicates a temperature indicator regulator. Table 1 shows the specifications of the heat exchanger. The total length (L) of each spiral element is 810m.
It was set as m.
試料は、低粘度液体には水を、高粘度液体には日本コン
スターチ■製酸糖化水アメ(サンシララフ85)を、濃
度75%に調整して使用した。(物性値は表2に記載)
圧力損失の測定およびスチームによる加熱試験、水道水
による冷却試験を行った。As for the samples, water was used as the low viscosity liquid, and acid saccharified starch syrup (Sansira Rough 85) manufactured by Nippon Konstarch ■ was used as the high viscosity liquid, and the concentration was adjusted to 75%. (Physical property values are listed in Table 2) Measurement of pressure loss, heating test with steam, and cooling test with tap water were conducted.
(3)試験結果 (3−1)低粘度液体による圧力損失 水道水を使用しての圧力損失の試験結果を図4に示す。(3) Test results (3-1) Pressure loss due to low viscosity liquid Figure 4 shows the pressure drop test results using tap water.
実施例の場合、比較例に対し圧力損失が小さく、流動性
の高い構造となっている。In the case of the example, the pressure loss is smaller than that of the comparative example, and the structure has high fluidity.
(3−2)低粘性液体による加熱試験
図5にはスチームによる水道水の加熱試験の結果を示し
た。j□は(2)(注1)式で与えられる。水道水のよ
うな低粘度性液体の場合、実施例と比較例とについて、
熱効率に顕著な差は見られないことがわかる。(3-2) Heating test using low viscosity liquid Figure 5 shows the results of a heating test on tap water using steam. j□ is given by equation (2) (Note 1). In the case of a low viscosity liquid such as tap water, regarding the examples and comparative examples,
It can be seen that there is no noticeable difference in thermal efficiency.
(3−3)高粘度液体による圧力損失
図61図7には、75%に調整した水アメの粘度vs剪
断速度、粘度vs温度の測定結果を示した。本試験では
、剪断速度の範囲はN−40〜20O8−1であり、こ
の範囲での粘度への影響は小さいが、温度の影響が大き
いことがわかる。(3-3) Pressure loss due to high viscosity liquid Figure 61 Figure 7 shows the measurement results of viscosity vs. shear rate and viscosity vs. temperature of starch syrup adjusted to 75%. In this test, the range of shear rate was N-40 to 20O8-1, and it can be seen that the influence on viscosity in this range is small, but the influence of temperature is large.
図8には、水アメを使用しての圧力損失の試験結果を示
した。水道水の場合と同様、水アメのような高粘性流体
においても同様な圧力損失の結果が得られた。FIG. 8 shows the pressure loss test results using starch syrup. Similar pressure drop results were obtained for high viscosity fluids such as starch syrup as in the case of tap water.
図9には、比較例の圧力損失の試験結果と7推測値との
比較を示した。推定値は(3)(注1〉式による。回転
粘度計により得られた粘度は実際の圧力損失より推定さ
れる値よりも小さい値となり。FIG. 9 shows a comparison between the pressure loss test results of the comparative example and the 7 estimated values. The estimated value is based on formula (3) (Note 1).The viscosity obtained by a rotational viscometer is a smaller value than the value estimated from the actual pressure loss.
その比は約0.60となる。以後、レイノルズ数にはこ
の粘度を用いて整理を行うものとする。The ratio is approximately 0.60. Hereafter, this viscosity will be used to organize the Reynolds number.
(3−4)高粘度液体による加熱試験
図10に水アメを使用してのスチームによる加熱試験結
果を示す。管内側伝熱係数hiは(I)(注1)式で与
えられ、φ−1,1とする。実施例の場合も比較例の場
合と同様、Reの1/3乗に比例し、係数Aは比較例の
場合1.85.実施例の場合1.28を得た。熱効率は
比較例の方が若干良いことがわかった。(3-4) Heating test using high viscosity liquid Figure 10 shows the results of a heating test using steam using starch syrup. The tube inside heat transfer coefficient hi is given by equation (I) (Note 1) and is set to φ-1,1. In the case of the example, as in the case of the comparative example, it is proportional to Re to the 1/3 power, and the coefficient A is 1.85 in the case of the comparative example. In the case of the example, 1.28 was obtained. It was found that the comparative example had slightly better thermal efficiency.
(3−5)高粘度液体による冷却試験 図IIには、水道水による冷却試験結果を示す。(3-5) Cooling test with high viscosity liquid Figure II shows the results of a cooling test using tap water.
比較例においては、加熱の場合と同様な結果が得られた
。実施例においては、 A−0,85で、加熱の場合よ
りも低い熱効率が得られた。In the comparative example, results similar to those obtained by heating were obtained. In the example, lower thermal efficiency was obtained at A-0,85 than in the case of heating.
(以下余白)
表1
表2
D推定値
つ日本コーンスターチ■テクニカル・サービス1こよる
データ
@添字0,1をそれぞれ管外側、管内側とする。また実
施例の水−加熱においてはr。−「1−oとする。(Leaving space below) Table 1 Table 2 D Estimated Value - Japan Cornstarch ■Technical Service 1 Data @ Subscripts 0 and 1 are the outside of the tube and the inside of the tube, respectively. In addition, r in the water-heating example. - “Let it be 1-o.
(4〉結果 (4−1)圧力損失 圧力損失については以下の結果を得た。(4>Results (4-1) Pressure loss Regarding pressure loss, the following results were obtained.
(i)低粘性液体(水) Re>104ΔP(実施例
)/ΔP(比較例)−0,40〜0,45(11)高粘
性液体(水アメ) Re<10ΔP(実施例)ノΔP
(比較例)−0,70〜0.75(4−2)熱交換効率
[jHコ (注2)熱交換効率については以下の結果を
得た。(i) Low viscosity liquid (water) Re>104ΔP (example)/ΔP (comparative example) -0,40 to 0,45 (11) High viscosity liquid (water syrup) Re<10ΔP (example) no ΔP
(Comparative example) -0.70 to 0.75 (4-2) Heat exchange efficiency [jHko (Note 2) The following results were obtained regarding heat exchange efficiency.
(1)低粘性液体(水)−スチーム加熱Re>103j
H(実施例)/j+(比較例)ζ1.001)高粘性液
体(水アメ) Re<10スチーム加熱jH(実施例
)/jH(比較例)ζ0.70冷却jH(実施例)/j
)l(比較例)ζ0゜50(5)考察
圧力損失については、実施例の熱交換器は、比較例に比
して0.75以下、特に低粘性液体の場合は0.45以
下である。(1) Low viscosity liquid (water) - steam heating Re>103j
H (Example) / j + (Comparative example) ζ 1.001) High viscosity liquid (water syrup) Re < 10 Steam heating jH (Example) / jH (Comparative example) ζ 0.70 Cooling jH (Example) / j
) l (Comparative example) ζ0゜50 (5) Consideration Regarding pressure loss, the heat exchanger of the example has a pressure loss of 0.75 or less compared to the comparative example, especially 0.45 or less in the case of low viscosity liquid. .
実施例の熱交換器は、水のような低粘性流体のスチーム
加熱の系の場合、比較例と同等の熱交換効率が得られる
。高粘性流体の場合においてもその簡易な構造及び低圧
力損失を考慮した上で使用可能である。In the case of a steam heating system for a low viscosity fluid such as water, the heat exchanger of the example can obtain heat exchange efficiency equivalent to that of the comparative example. Even in the case of high viscosity fluid, it can be used in consideration of its simple structure and low pressure loss.
(以下余白)
(注1 ) (1)、(2)、(3)式%式%
()
(2)
(3)
()
()
管内側流体の流量をW <kg/h)とすると熱交換量
Q (kcal/h)は
Q−W−C・Δt(C:比熱) (■)飽和蒸
気表の基に、スチーム2次圧よりエンタルピーh (k
cal/kg)を読みとり、スチーム流量W′(kg/
h)を次式より求める。(Left below) (Note 1) (1), (2), (3) formula % formula % () (2) (3) () () If the flow rate of the fluid inside the pipe is W < kg/h), the heat The exchange rate Q (kcal/h) is Q-W-C・Δt (C: specific heat) (■) Based on the saturated steam table, the enthalpy h (kcal/h) is calculated from the secondary pressure of steam.
cal/kg) and check the steam flow rate W' (kg/kg).
h) is obtained from the following formula.
W’ −Q/h (I
II)また9次式より総括伝熱係数U (kcal/r
r?・h・℃)を求め。W'-Q/h (I
II) Also, the overall heat transfer coefficient U (kcal/r
r?・h・℃).
U−Q/A・ΔtIIl(Δt;対数平均温度差)(■
)(1)式よりhlを算出する。さらにり2)式より」
Hを求める。但しり。は計算式を用いて求める。U-Q/A・ΔtIIl (Δt; logarithmic average temperature difference) (■
) Calculate hl from equation (1). Furthermore, from formula 2)
Find H. However. is calculated using a calculation formula.
(冷却)
冷却水流ffiW(kg/h)を実測し、以下スチーム
加熱の場合と同様にしてhlを求める。(Cooling) The cooling water flow ffiW (kg/h) is actually measured, and hl is determined in the same manner as in the case of steam heating.
(以下余白)(Margin below)
図IA、B、Cは管体(内管)の構造を示す側断面図で
あって2図IAは実施例に係るもの1図IBは比較例に
係るもの2図ICはエレメントを備えていない単なる空
管に係るもの。
図1−1は実施例の熱交換器を示した側断面図及びその
C−C断面図(エレメントを除いて比較例等も同様)。
図1−2は試験に用いた熱交換フローを示した図
図2.3は高粘度液体としての水アメの特性(比重、比
熱)を示すグラフ。
図4は低粘度液体による圧力損失の結果を示すグラフ。
図5は低粘度液体による加熱試験の結果を示すグラフ。
第6.7図は高粘度液体としての水アメについて、粘度
vs剪断速度、粘度vs温度の関係を示すグラフ。
図8,9は高粘度液体による圧力損失の結果を示すグラ
フ。
叉10は高粘度液体による加熱試験の結果を示すグラフ
。
図11は高粘度液体による冷却試験の結果を示すグラフ
。
を夫々表わす。
1・・・螺旋エレメント
1a・・・単位エレメント
2・・・内管 3・・・外管第1A図
第1B図Figures IA, B, and C are side sectional views showing the structure of the tube body (inner tube), and 2 Figure IA is related to the example 1 Figure IB is related to the comparative example 2 Figure IC is not equipped with an element Items related to simple empty pipes. FIG. 1-1 is a side sectional view showing the heat exchanger of the example and its CC sectional view (the same applies to the comparative example except for the element). Figure 1-2 shows the heat exchange flow used in the test. Figure 2.3 is a graph showing the characteristics (specific gravity, specific heat) of starch syrup as a high viscosity liquid. FIG. 4 is a graph showing the results of pressure loss due to low viscosity liquid. FIG. 5 is a graph showing the results of a heating test using a low viscosity liquid. Figure 6.7 is a graph showing the relationship between viscosity vs. shear rate and viscosity vs. temperature for starch syrup as a high viscosity liquid. 8 and 9 are graphs showing the results of pressure loss due to high viscosity liquid. 10 is a graph showing the results of a heating test using a high viscosity liquid. FIG. 11 is a graph showing the results of a cooling test using a high viscosity liquid. respectively. 1... Helical element 1a... Unit element 2... Inner tube 3... Outer tube Figure 1A Figure 1B
Claims (4)
備え、 螺旋エレメントが、捻り角度180゜を有する複数の単
位エレメントを接続角度0゜で連続してなり、 隣接する単位エレメントが逆方向の捻りになっている、 ことを特徴とする熱交換用管体。(1) A helical element that extends in the longitudinal direction in the pipe, the helical element is made up of a plurality of unit elements each having a twist angle of 180° connected at a connection angle of 0°, and adjacent unit elements are twisted in the opposite direction. A heat exchange tube body characterized by:
は二以上の内管とからなり、 内管内において長手方向に延びる螺旋エレメントを備え
、 螺旋エレメントが、捻り角度180゜を有する複数の単
位エレメントを接続角度0゜で連続してな隣接する単位
エレメントが逆方向の捻りになっている。 ことを特徴とする熱交換器。(2) Consisting of an outer tube and one or more inner tubes disposed with a gap within the outer tube, comprising a helical element extending in the longitudinal direction within the inner tube, the helical element having a twist angle of 180°. A plurality of unit elements are connected consecutively at a connection angle of 0°, and adjacent unit elements are twisted in opposite directions. A heat exchanger characterized by:
ズ数)の低粘性液体である請求項1又は2記載の管体又
は熱交換器。(3) The tube body or heat exchanger according to claim 1 or 2, wherein the heat exchange medium is a low viscosity liquid with Re>10^4 (Re: Reynolds number).
請求項1又は2記載の管体又は熱交換器。(4) The tube body or heat exchanger according to claim 1 or 2, wherein the helical element is joined to the inner wall of the tube by brazing.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP9190A JPH03204592A (en) | 1990-01-05 | 1990-01-05 | Heat exchanger |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP9190A JPH03204592A (en) | 1990-01-05 | 1990-01-05 | Heat exchanger |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH03204592A true JPH03204592A (en) | 1991-09-06 |
Family
ID=11464449
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP9190A Pending JPH03204592A (en) | 1990-01-05 | 1990-01-05 | Heat exchanger |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH03204592A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5307867A (en) * | 1992-08-10 | 1994-05-03 | Noritake Co., Limited | Heat exchanger |
Citations (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS50150055A (en) * | 1974-05-23 | 1975-12-01 | ||
| JPS57120097A (en) * | 1981-01-20 | 1982-07-26 | Mitsubishi Heavy Ind Ltd | Heat exchanger |
| JPS6158590B2 (en) * | 1981-12-09 | 1986-12-12 | Kanebo Ltd | |
| JPS635277B2 (en) * | 1985-04-22 | 1988-02-02 | Canon Kk |
-
1990
- 1990-01-05 JP JP9190A patent/JPH03204592A/en active Pending
Patent Citations (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS50150055A (en) * | 1974-05-23 | 1975-12-01 | ||
| JPS57120097A (en) * | 1981-01-20 | 1982-07-26 | Mitsubishi Heavy Ind Ltd | Heat exchanger |
| JPS6158590B2 (en) * | 1981-12-09 | 1986-12-12 | Kanebo Ltd | |
| JPS635277B2 (en) * | 1985-04-22 | 1988-02-02 | Canon Kk |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5307867A (en) * | 1992-08-10 | 1994-05-03 | Noritake Co., Limited | Heat exchanger |
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